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000320884 0247_ $$2doi$$a10.1016/S0550-3213(01)00544-2
000320884 0247_ $$2ISSN$$a0550-3213
000320884 0247_ $$2ISSN$$a1873-1562
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000320884 037__ $$aPUBDB-2017-02160
000320884 041__ $$aEnglish
000320884 082__ $$a530
000320884 0881_ $$ahep-ex/0106070; DESY-01-062
000320884 088__ $$2arXiv$$ahep-ex/0106070
000320884 088__ $$2DESY$$aDESY-01-062
000320884 1001_ $$aAdloff, C.$$b0
000320884 245__ $$aPhotoproduction with a leading proton at HERA
000320884 260__ $$aAmsterdam$$bNorth-Holland Publ. Co.$$c2001
000320884 3367_ $$2DRIVER$$aarticle
000320884 3367_ $$2DataCite$$aOutput Types/Journal article
000320884 3367_ $$0PUB:(DE-HGF)29$$2PUB:(DE-HGF)$$aReport$$mreport
000320884 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1497422480_25977
000320884 3367_ $$2BibTeX$$aARTICLE
000320884 3367_ $$2ORCID$$aJOURNAL_ARTICLE
000320884 3367_ $$00$$2EndNote$$aJournal Article
000320884 520__ $$aThe total cross section for the photoproduction process with a leading proton in the final state has been measured at γp  centre-of-mass energies  W of 91, 181 and 231 GeV. The measured cross sections apply to the kinematic range with the transverse momentum of the scattered proton restricted to p T ⩽0.2 GeV and 0.68⩽ z ⩽0.88, where z = E p ′/ E p is the scattered proton energy normalised to the beam energy. The cross section d σ γp → Xp ′ ( W , z )/d z is observed to be independent of  W and z within the measurement errors and amounts to (8.05±0.06 ( stat )±0.89 ( syst )) μb on average. The data are well described by a Triple Regge model in which the process is mediated by a mixture of exchanges with an effective Regge trajectory of intercept α i (0)=0.33±0.04 ( stat )±0.04 ( syst ) . The total cross section for the interaction of the photon with this mixture ( γα i → X ) can be described by an effective trajectory of intercept α k (0)=0.99±0.01 ( stat )±0.05 ( syst ) . Predictions based on previous triple Regge analyses of pp → pX data assuming vertex factorisation are broadly consistent with the γp data. The measured cross sections are compared with deep inelastic scattering leading proton data in the same region of  z and p T for photon virtuality Q 2 >2.5 GeV 2 . The ratio of the cross section for leading proton production to the total cross section is found to rise with  Q 2 .
000320884 536__ $$0G:(DE-HGF)POF3-899$$a899 - ohne Topic (POF3-899)$$cPOF3-899$$fPOF III$$x0
000320884 588__ $$aDataset connected to CrossRef, INSPIRE
000320884 650_7 $$2INSPIRE$$apositron p: colliding beams
000320884 650_7 $$2INSPIRE$$apositron p: deep inelastic scattering
000320884 650_7 $$2INSPIRE$$apositron p: inclusive reaction
000320884 650_7 $$2INSPIRE$$aphoton: dissociation
000320884 650_7 $$2INSPIRE$$ahadron: photoproduction
000320884 650_7 $$2INSPIRE$$ap: leading particle
000320884 650_7 $$2INSPIRE$$ap: energy
000320884 650_7 $$2INSPIRE$$aexchange: Regge
000320884 650_7 $$2INSPIRE$$adifferential cross section: energy dependence
000320884 650_7 $$2INSPIRE$$aRegge poles: triple-Regge limit
000320884 650_7 $$2INSPIRE$$amomentum transfer dependence
000320884 650_7 $$2INSPIRE$$aH1
000320884 650_7 $$2INSPIRE$$aforward spectrometer: experimental results
000320884 650_7 $$2INSPIRE$$aDESY HERA Stor
000320884 650_7 $$2INSPIRE$$apositron p --> p positron anything
000320884 650_7 $$2INSPIRE$$aapprox. 300 GeV-cms
000320884 693__ $$0EXP:(DE-588)4443767-5$$1EXP:(DE-588)4159571-3$$5EXP:(DE-588)4443767-5$$aHERA$$eHERA: H1$$x0
000320884 7001_ $$aAndreev, V.$$b1
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